(d) From Einstein equation $E = W_{0} + \frac{1}{2}mv^{2}$
$\sqrt{\frac{2(E - W_{0})}{m}} = v$
and a charged particle placed in uniform magnetic field experience a force
$F = \frac{mv^{2}}{r} \Rightarrow evB = \frac{mv^{2}}{r} \Rightarrow r = \frac{mv}{eB}$
$\Rightarrow r = \frac{\sqrt{2m(E - W_{0})}}{eB}$